2005
DOI: 10.1080/14689360412331313039
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The invariant manifold structure of the spatial Hill's problem

Abstract: The paper studies the invariant manifolds of the spatial Hill's problem associated to the two liberation points. A combination of analytical and numerical tools allow the normalization of the Hamiltonian and the computation of periodic and quasi-periodic (invariant tori) orbits. With these tools, it is possible to give a complete description of the center manifolds, association to the liberation points, for a large set of energy values.A systematic exploration of the homoclinic and heteroclinic connections bet… Show more

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Cited by 41 publications
(44 citation statements)
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“…We only pay attention to two among the variety of families of periodic orbits of the Hill problem that are known to exist for variations of the Jacobi constant [6,7]. These are the family of 8-shaped periodic orbits, which starts from small vertical oscillations through the L 2 collinear point, and the family of Halo orbits, which bifurcates from the family of Lyapunov orbits that starts from small retrograde oscillations in the plane of the primaries about L 2 .…”
Section: Hill Problem Dynamicsmentioning
confidence: 99%
“…We only pay attention to two among the variety of families of periodic orbits of the Hill problem that are known to exist for variations of the Jacobi constant [6,7]. These are the family of 8-shaped periodic orbits, which starts from small vertical oscillations through the L 2 collinear point, and the family of Halo orbits, which bifurcates from the family of Lyapunov orbits that starts from small retrograde oscillations in the plane of the primaries about L 2 .…”
Section: Hill Problem Dynamicsmentioning
confidence: 99%
“…The two orbits With the Floquet's Theory, their linear stabilities can be evaluated; a PO is stable if all the eigenvalues of its monodromy matrix have unity magnitude (Chicone 1999). Following (Gómez et al 2005), the monodromy matrix of a PO usually has the eigenvalues in the form of {1, 1, λ 1 , 1/λ 1 , λ 2 , 1/λ 2 }, the stability index is commonly defined as s i = |λ i + 1/λ i |, i = 1, 2. The PO is linearly stable if s i < 2, while linearly unstable if s i > 2.…”
Section: Pos In the Non-averaged Modelmentioning
confidence: 99%
“…The problem is of three degrees of freedom, yet admitting the Jacobi constant H = −C/2. Insight regarding stability in Hill model is available through the computation of families of periodic orbits in the rotating frame [48,16,13], where information on the stability character of each periodic orbit is easily obtained [15,2,18]. Planar, retrograde periodic orbits are generally stable, and, on the contrary, corresponding planar, direct periodic orbits change to instability relatively close to the central body [48,16,17,31].…”
Section: Spatial Hill Model Dynamics 21 Hamiltonian Of the Problem Amentioning
confidence: 99%